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College Physics for AP® Courses

23.10 RL Circuits

College Physics for AP® Courses23.10 RL Circuits

Learning Objectives

By the end of this section, you will be able to:

  • Calculate the current in an RL circuit after a specified number of characteristic time steps.
  • Calculate the characteristic time of an RL circuit.
  • Sketch the current in an RL circuit over time.

We know that the current through an inductor LL size 12{L} {} cannot be turned on or off instantaneously. The change in current changes flux, inducing an emf opposing the change (Lenz’s law). How long does the opposition last? Current will flow and can be turned off, but how long does it take? Figure 23.44 shows a switching circuit that can be used to examine current through an inductor as a function of time.

Part a of the figure shows an inductor connected in series with a resistor. The arrangement is connected across a cell by an on and off switch with two positions. When in position one, the battery, resistor, and inductor are in series and a current is established. In position two, the battery is removed and the current stops eventually because of energy loss in the resistor. Part b of the diagram shows the graph when the switch is in position one. It shows a graph for current growth verses time. The current is along the Y axis and the time is along the X axis. The graph shows a smooth rise from origin to a maximum value I zero corresponding to Y axis and value four tau on X axis. Part c of the diagram shows the graph when the switch is in position two. It shows a graph for current decay verses time is shown. The current is along the Y axis and the time is along the X axis. The graph is decreasing curve from a value I zero on Y axis, touching the X axis at a point where value of time equals four tau.
Figure 23.44 (a) An RL circuit with a switch to turn current on and off. When in position 1, the battery, resistor, and inductor are in series and a current is established. In position 2, the battery is removed and the current eventually stops because of energy loss in the resistor. (b) A graph of current growth versus time when the switch is moved to position 1. (c) A graph of current decay when the switch is moved to position 2.

When the switch is first moved to position 1 (at t=0t=0 size 12{t=0} {}), the current is zero and it eventually rises to I0=V/RI0=V/R size 12{I rSub { size 8{0} } = ital "V/R"} {}, where R R is the total resistance of the circuit. The opposition of the inductor LL size 12{L} {} is greatest at the beginning, because the amount of change is greatest. The opposition it poses is in the form of an induced emf, which decreases to zero as the current approaches its final value. The opposing emf is proportional to the amount of change left. This is the hallmark of an exponential behavior, and it can be shown with calculus that

I=I0(1et/τ)    (turning on),I=I0(1et/τ)    (turning on), size 12{I=I rSub { size 8{0} } \( 1 - e rSup { size 8{ - t/τ} } \) } {}
23.45

is the current in an RL circuit when switched on (Note the similarity to the exponential behavior of the voltage on a charging capacitor). The initial current is zero and approaches I0=V/RI0=V/R size 12{I rSub { size 8{0} } = ital "V/R"} {} with a characteristic time constant τ τ for an RL circuit, given by

τ=LR,τ=LR, size 12{τ= { {L} over {R} } } {}
23.46

where ττ size 12{τ} {} has units of seconds, since 1 H = 1 Ω · s 1 H = 1 Ω · s . In the first period of time ττ size 12{τ} {}, the current rises from zero to 0.632I00.632I0 size 12{0 "." "632"I rSub { size 8{0} } } {}, since I=I0(1e1)=I0(10.368)=0.632I0I=I0(1e1)=I0(10.368)=0.632I0 size 12{I=I rSub { size 8{0} } \( 1 - e rSup { size 8{ - 1} } \) =I rSub { size 8{0} } \( 1 - 0 "." "368" \) =0 "." "632"I rSub { size 8{0} } } {}. The current will go 0.632 of the remainder in the next time ττ size 12{τ} {}. A well-known property of the exponential is that the final value is never exactly reached, but 0.632 of the remainder to that value is achieved in every characteristic time ττ size 12{τ} {}. In just a few multiples of the time ττ size 12{τ} {}, the final value is very nearly achieved, as the graph in Figure 23.44(b) illustrates.

The characteristic time ττ size 12{τ} {} depends on only two factors, the inductance LL size 12{L} {} and the resistance RR size 12{R} {}. The greater the inductance LL size 12{L} {}, the greater ττ size 12{τ} {} is, which makes sense since a large inductance is very effective in opposing change. The smaller the resistance RR size 12{R} {}, the greater ττ size 12{τ} {} is. Again this makes sense, since a small resistance means a large final current and a greater change to get there. In both cases—large LL size 12{L} {} and small RR size 12{R} {} —more energy is stored in the inductor and more time is required to get it in and out.

When the switch in Figure 23.44(a) is moved to position 2 and cuts the battery out of the circuit, the current drops because of energy dissipation by the resistor. But this is also not instantaneous, since the inductor opposes the decrease in current by inducing an emf in the same direction as the battery that drove the current. Furthermore, there is a certain amount of energy, (1/2)LI02(1/2)LI02 size 12{ \( "1/2" \) ital "LI" rSub { size 8{0} } rSup { size 8{2} } } {}, stored in the inductor, and it is dissipated at a finite rate. As the current approaches zero, the rate of decrease slows, since the energy dissipation rate is I2RI2R size 12{ I rSup { size 8{2} } R} {}. Once again the behavior is exponential, and II is found to be

I=I0et/τ    (turning off).I=I0et/τ    (turning off). size 12{I=I rSub { size 8{0} } e rSup { size 8{ - t/τ} } } {}
23.47

(See Figure 23.44(c).) In the first period of time τ=L/Rτ=L/R size 12{τ=L/R} {} after the switch is closed, the current falls to 0.368 of its initial value, since I=I0e1=0.368I0I=I0e1=0.368I0 size 12{I=I rSub { size 8{0} } e rSup { size 8{ - 1} } =0 "." "368"I rSub { size 8{0} } } {}. In each successive time ττ size 12{τ} {}, the current falls to 0.368 of the preceding value, and in a few multiples of ττ size 12{τ} {}, the current becomes very close to zero, as seen in the graph in Figure 23.44(c).

Example 23.9

Calculating Characteristic Time and Current in an RL Circuit

(a) What is the characteristic time constant for a 7.50 mH inductor in series with a 3.00 Ω 3.00 Ω resistor? (b) Find the current 5.00 ms after the switch is moved to position 2 to disconnect the battery, if it is initially 10.0 A.

Strategy for (a)

The time constant for an RL circuit is defined by τ=L/Rτ=L/R size 12{τ=L/R} {}.

Solution for (a)

Entering known values into the expression for ττ size 12{τ} {} given in τ=L/Rτ=L/R size 12{τ=L/R} {} yields

τ=LR=7.50 mH3.00Ω=2.50 ms.τ=LR=7.50 mH3.00Ω=2.50 ms. size 12{τ= { {L} over {R} } = { {7 "." "50"" mH"} over {3 "." "00 " %OMEGA } } =2 "." "50"" ms"} {}
23.48

Discussion for (a)

This is a small but definitely finite time. The coil will be very close to its full current in about ten time constants, or about 25 ms.

Strategy for (b)

We can find the current by using I=I0et/τI=I0et/τ size 12{I=I rSub { size 8{0} } e rSup { size 8{ - t/τ} } } {}, or by considering the decline in steps. Since the time is twice the characteristic time, we consider the process in steps.

Solution for (b)

In the first 2.50 ms, the current declines to 0.368 of its initial value, which is

I = 0.368I0=(0.368)(10.0 A) = 3.68 A at t=2.50 ms. I = 0.368I0=(0.368)(10.0 A) = 3.68 A at t=2.50 ms.
23.49

After another 2.50 ms, or a total of 5.00 ms, the current declines to 0.368 of the value just found. That is,

I = 0.368I=(0.368)(3.68 A) = 1.35 A at t=5.00 ms.I = 0.368I=(0.368)(3.68 A) = 1.35 A at t=5.00 ms.alignl { stack { size 12{ { {I}} sup { ' }=0 "." "368"I= \( 0 "." "368" \) \( 3 "." "68"" A" \) } {} # size 12{" "=1 "." "35"" A at "t=5 "." "00"" ms"} {} } } {}
23.50

Discussion for (b)

After another 5.00 ms has passed, the current will be 0.183 A (see Exercise 23.69); so, although it does die out, the current certainly does not go to zero instantaneously.

In summary, when the voltage applied to an inductor is changed, the current also changes, but the change in current lags the change in voltage in an RL circuit. In Reactance, Inductive and Capacitive, we explore how an RL circuit behaves when a sinusoidal AC voltage is applied.

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